First-principles calculations show that the defect pair (2V(Cu)(-) + I
n-Cu(+)) in CuInSe2 has an unusually low formation energy, due both to
the relative ease of forming Cu vacancies (V-Cu) and to the attractiv
e interactions between V(Cu)(-) and In-Cu(2+). The defect pair is pred
icted to be electrically inactive. This explains the surprising electr
ical tolerance of CuInSe2 to its huge (similar to 1%) concentration of
native defects. An attractive interaction among the defect pairs is f
urther predicted to lead to a crystallographic ordering of the pairs,
explaining the observed, but hitherto surprising, structures CuIn5Se8,
CuIn3Se5, Cu2In4Se7, etc.